Well logging radiation sources



Jan. 1, 1963 R. E. FEARON ETAL 3,071,690

WELL LOGGING RADIATION SOURCES Original Filed July 30, 1949 4 Sheets-Sheet 1 AMPLIFIER SHAPER 4 38 45 v PULSE 44 CONDITIONLN CIRCUITS I DETECTOR POWER SUPPLY OBSTACLE INVENTORS ROBERT E. FEARON BY JEAN M. THAY ER jy. 1 marm/emkzv ATTORNEY Jan. 1, 1963 R. E. FEARON ET AL 3,071,590

WELL LOGGING RADIATION SOURCES Original Filed July 30, 1949 4 Sheets-Sheet 2 TO SURFACE IMPEDANCE MATCH 37 SHAPER 36 j l I n SCALING /35 A R AMPL. 34

f 8 d DISCRIM 33 I INATOR E 0 A FUNCTION OF INTENSITY OBSTACLE INVENTORS ROBERT E. FEARON 4 SOURCE OF JEAN M. THAYER @467 2 UT 0N5 MKM ATTOR NEY Jan. 1, 1963 Original Filed July 30, 1949 POWER 8 U PP LY R. E. FEARON ETAL WELL LOGGING RADIATION SOURCES 4 Sheets-Sheet 3 VOLTAGE SOURCE POWER 5U PP LY INVENTORS ROBERT E. FEARON JEAN M. THAYER w /Mmw,

AT TOR NEY Jan. 1, 1963 R. E. FEARON ETAL 3,071,690

WELL LOGGING RADIATION SOURCES Original Filed July 30, 1949 4 Sheets-Sheet 4 VOLTAG E SOURCE INVENTORS ROBERT E. FEARON JEAN M. THAYER ATTORNEY Patented Jan. 1, 1%3

3,071,690 WELL LOGGING RADiATlON SOURCES Robert E. Fear-on and Jean M. Thayer, Tuisa, Gilda, assignors to Weil tiurveys, lnc., a corporation of Betaware Original application July 30, 1949, Ser. No. 1il7,8ii6, now Patent No. 2,712,081, dated June 28, 1955. Divided and this application Apr. 19, 1954, Ser. No. 423,969 16 Claims. ((11. 250-645) This invention relates generally to a method and apparatus for identifying substances existing in difficultly accessible locations, for example, adjacent to a deep narrow drill hole, and more particularly to a method and apparatus for identifying and distinguishing these substances from each other by nuclear reactions in the substances. This is a division of our copending application, Serial No. 107,806, filed July 30, 1949, for a Method for Neutron Well Logging, now US. Patent 2,712,081.

This invention is directed to the solution of a problem which has been long recognized by geologists and geophysicists, and by others, confronted with the problem of locating valuable substances, such as petroleum, in the sub-surface formations of the earth. The problem of discovering with certainty the existence of a particularly valuable substance in the sub-surface formations of the earth has only been partially solved by the prior art workers. All prior efforts to solve the problem have met with failure for the reason that no parameter could be found which was solely characteristic of the valuable substances that it was desired to locate. As an example, in the art of well logging a partial solution to the problem goes as far as determining with certainty that either salt water or petroleum exists in a particular formation but a complete solution is not possible, since prior to this invention, no parameter was known whereby the two substances could be distinguished, in situ, from each other.

Numerous other methods advanced by the workers in the prior art for locating valuable substances in the subsurface formations of the earth include: electrical methods which involve the measurement of self-potential, conductivity, and resistivity; thermal methods; seismic methods which treat of the acoustical properties of the subsurface formations; natural radioactivity of the formations; and those methods in which the formations are irradiated with radioactive radiations and an effect such as the gamma radiation produced by the neutron interactions in the formations measured. All of these methods as well as others which have not been enumerated above, have not afforded a complete solution to the above problem in that none of them measures a parameter that is solely characteristic of the valuable substances that one is desirous of locating.

For the purpose of particularly describing and setting forth the respects in which this invention differs from and represents advancement upon the prior art, there is set forth a description of the efiorts of previous workers insofar as they have been directed to the problem which has been stated in the previous paragraph.

The location of petroleum has been attempted by various well logging methods which are sensitive to some physical characteristic imparted to the rocks by the presence of petroleum in them. For example, resistivity methods in combination with other methods somewhat ambiguously enable detection of petroleum. The inconvenience and uncertainty of the use of resistivity methods arise from the fact that resistivity is a general property of rocks, and is possessed by some rocks not containing petroleum to an even greater extent than the degree to which the property is manifested by certain other rocks full of petroleum. For example, Indiana limestone will be found to have a much higher resistivity than oil saturated sandstone of the Frio formation in the Gulf Coast oil fields. Furthermore, sandstone which contains natural gas, has a high resistivity, as does also coal. Moreover, limestone may show a decrease of resistivity where an oil bearing horizon appears. It could similarly be shown how each and every one of the other non-nuclear logging methods have specific shortcomings which analogously prevent them from being or amounting to a specific recognition of petroleum.

In the art of nuclear well logging, to which this invention belongs, particular attention is called to the method described by John C. Bender in his United States patent, No. 2,133,776, in which he recites a method of observing secondary radiations caused by exposing the formations adjacent to a bore hole to primary radiation, such as X-rays and radiations of radium and uranium. The property of matter which one would observe in carrying out the disclosure of Bender can be said to be related to electrons in the matter. This property is shared by all substances to a greater or lesser degree, and is not, therefore, capable of making a specific distinction of petroleum.

There are also two methods which have been previously discovered and disclosed in United States patents, Nos. 2,308,361 and 2,349,712, by Robert E. Fearon, in which is described bombarding the strata of the earth adjacent to a bore hole with neutrons and observing any secondary rays that may be produced from the formations as influenced by the bombardment. This capacity of material to react with neutrons and give secondary rays of several sorts is a common and highly distributed property possessed by the substances of the earth. These methods, moreover, enable measurements to be made which are specifically influenced by the presence of hydrogen. The way in which the influence of hydrogen comes into play in these previous inventions, is through its ability to partially prevent neutrons from a source, separated from a detector of secondary radiation, from arriving in the vicinity of the detector. Without arriving in the vicinity of the detector, they are, of course, unable to react upon general characteristics of the matter there present, or produce secondary rays of any nature.

The specific indication of hydrogen through this phenomenon, which occurs in the practice of the above mentioned patents. is the nearest approach to a direct observation of petroleum. The recognition of hydrogen, desirable though it is, falls short of the solution of the problem of identifying petroleum, because of the presence of hydrogen in nearly all porous strata. The hydrogen combined with oxygen, as water, is generally present in porous strata. The shales also are very rich in hydrogen though non-porous and not usually a source'of petroleum. To secure a specific recognition of petroieum'will require some kind of observation or systems of observations which would reiate themselves more specifically to its occurrence.

Folkert Brons has set forth in his United States patent, No. 2,220,509, a method generally similar to the above two methods in which the observations are ascribed to that form of secondary radiation which comprises slow neutrons. He provides that his observation be based upon the detection of those neutrons which have been diffused, or slowed down, by interactions with elements in the strata of low atomic weight. He effects his measurements by producing, in the detector of radiation, disintegration products resulting from the reaction of his slow neutrons with the atomic nuclei which are there present, and detecting these disintegration products as an indication of the presence of slowed-down neutrons. As specified by Brons, his method of observing a particular class of secondary radiation, caused by neutron bombardment, is particularly sensitive to the presence in the strata of atoms among which the neutrons may diffuse, and which are of low atomic weight. Since the most outstanding example of low atomic weight atoms in the earth, is the element hydrogen, the property to be observed by Brons will, like the previous inventions of Robert E. Fearon, give particular emphasis to hydrogen. The general weaknesses of these methods are thus apparent, as they are applied to the problem of identification of petroleum.

Russell has disclosed, in his United States patent, No. 2,469,462, a method of making observations which rely upon certain other properties of strata enabling him to perform measurements which ignore the concentration of hydrogen present therein. These other properties, thus observed, will obviously correspond with ditferent geological factors and will correlate differently than is the case for methods which are preeminently hydrogensensitive.

As Russell states, his log indicates the presence of and evaluates other variable alfecting the usual neutron log, such as an increase or decrease in hardness or intensity of the gamma rays of neutron capture which al most necessarily occurs with a change in concentration of the elements chiefly responsible for capture.

It may be set forth that Russells method, if practiced in accordance with his specification, will be particularly sensitive to the extent of neutron capture for neutrons of high energy. This is true since he makes his observa tion, among other things, at a distance at which the rate of production of degraded neutrons of low energy has not risen to the value expected for large thicknesses of matter. Thus, in his case, there are in the vicinity of the detector of radiation, a relatively larger population of energetic neutrons, and the effects of these neutrons on the detector are therefore more likely and are relatively emphasized. Now it is the nature of his invention, from the standpoint of nuclear physics, that the reactions of carbon with neutrons are quite improbable. It is not, therefore, to be expected that Russell could, by his method, recognize petroleum except ambiguously through his provision of means sensitive to the presence of hydrogen, which he has also set forth in this patent.

Therefore, this patent of Russells like the others enumerated above, falls in the general class of nuclear methods not giving specific recognition of petroleum, and, because of this shortcoming, does not represent a complete solution to the problem which has been recited.

In his United States Patent 2,469,463, Russell has specified means of measuring and comparing several additional factors in neutron well logging, which are not primarily or chiefly related to hydrogen content. It might be said that in this invention, Russell has set forth a means of measuring the factor C, which has been defined, and to which significance has been attributed in column 1, page 37 of volume 4, No. 6, Nucleonics, June 1949. As can be seen from consideration of this published discussion of this factor, it will not be easy to measure, because of its relatively small variations from one rock type to another. Furthermore, specifically, there is nothing especially: indicativeof petroleum which will influence this factor. Unfortunately, contrary to Russells statements, the ability of hydrogen to capture neutrons is quite appreciable, when compared with other elements commonly present in the earth. Also, hydrogen stands apart among the elements of the earth in that it emits uncommonly little gamma-ray energy per neutron which it captures. For these reasons, the practice of Russells Patent 2,469,463, Will still result in a measurement which is preeminently affected by hydrogen, and which is therefore unable to specifically identify petroleum, and does not represent the solution to the problem to which this invention is directed.

Russells patent, No. 2,469,461, is a method of studying density by scattering of gamma rays from subsurface strata. There is no indication that there is any specific correlation between density and the occurrence of fluid 7 1n the pore spaces of rocks. Too many factors unr lat to the occurrence of fluid have a larger efiect on density. Kind of rock minerals predominantly present, amount of cementation, amount of pore space, all have a great effect, and prevent Russells gamma ray scattering procedure from being used as a method of specifically iden tifying petroleum. This invention of Russell therefore also falls short of being a solution to the problem to which the present invention is directed.

The instant invention provides a complete solution to the above problem. This solution consists of a system of observations by which the operator is enabled to recognize and quantitatively measure nuclear species of the subsurface formations adjacent a bore hole. Although the desired substances quite often are not elements or single nuclear species, the chemical laws of combining proportions enable accurate appraisal of such things as the occurrence of petroleum. Recognition of nuclear species is accomplished by subjecting the substance adjacent to the bore hole to bombardment with penetrating radiations of a nature to cause specific and determinative quantized changes in the potential energy of the said nuclear species. These quantized energy changes which are specific to the particular kinds of atoms to be determined are used as a means of recognizing the desired atoms, which recognition is accomplished by means of selective neutron detection, selective for specific energy ranges of neutrons, and/or specific limits of direction of incidence and sense of direction of incidence.

Among the means which are required for the solution of the above problem, there is provided exceedingly powerful and energetically efiicient monoenergetic neutron sources, relying upon the nucear reactions caused by electrically or electromagnetically accelerated particles. These are provided in a form which is adapted to be lowered into abore hole, and employed therein to bombard the ro ks adjacent to the bore hole. Also required for the practice of this invention are powerful capsuled neutron-emitting sources, depending for their operation upon energetic particles emitted by radioactive substances. There is set forth the manner of choosing and designing such neutron-emitting sources, showing how a person skilled in the art can avail himself of intensities hundreds of times greater than those which are now available.

Requiring in the practice of this method are various means of observing neutrons which permit the determination of the energy, the direction of incidence of neutrons, and the sense of direction.

Among these means, there are provided devices which determine both energy and direction of incident neutrons within certain limits. There is also provided a device for detecting phenomena described in nuclear physics as n-p reactions. This device enables exact determination of energy of neutrons, and a somewhat ambiguous determination of direction. Incidental to the practice of this invention also is a device for resolving nuclear data which gives only a general indication of energy, and interpretating this general indication of the energy of neutrons in a more exact way. There is also provided, as a means of practicing this invention, a choice of the manner of employment of a number of neutron filters adapted to select specific energy groups of neutrons. It is shown how these filters may be employed for the purpose of identifying specific elements in the strata.

Therefore the primary object of this invention is the provision of a method and apparatus for identifying valuable substances by separately measuring the influence of specific properties of the nuclei of the valuable substances upon a flux of fast neutrons.

Another important object of this invention is the pro vision of a method and apparatus whereby petroleum can be positively identified in the subsurface strata adjacent a bore hole.

This invention also contemplates a method and means for locating valuable substances situated in difiicultly accessible locations by identifying and measuring the inthe formations.

Another object is to provide a novel monoenergetic neutron source which is compact and permanently enclosed.

Still another object is to provide a novel radiation source of the above type that will produce 17 m.e.v. (million electron volt) gamma rays.

Other objects and advantages of the present invention will become apparent from the following detailed description when considered with the drawings, in which FIGURE 1 is a schematic illustration of a well logging operation showing the surface recording system;

FIGURE 2 is a diagrammatic illustration of a subsurface instrument with the detector illustrated in vertical section;

FIGURE 3 illustrates the type of well log that would be produced by the present invention;

FIGURE 4 is a fragmentary sectional view of a subsurface instrument showing one of the novel neutron sources, contemplated by this invention, in operative position therein;

FIGURE 5 illustrates diagrammatically a modified form of neutron source;

FIGURE 6 illustrates diagrammatically still another modified neutron source.

As pointed out above, consideration of the problem of well logging has led to the conclusion that there is a necessity for the discovery of methods which will identify more specifically the substances found in the rocks adjacent to wells which are logged. Specific identifying properties, which could be relied upon as a means of recognition of substances, must be able to cause an efiect which is observable under the logging conditions which prevail. Preferably the process making the observations possible should be one which acts through space and through matter which fills the space between the position in which the rock to be identified is found, and the location of the detecting apparatus in the bore hole. The necessity for acting through space arises because of the prevalence of casing and/or cement and/or fluid of various sorts which commonly exit in the well bores, and which interfere with the measuring process. Another reason why considerable action through space is essential is the need for the depth of investigation to be adequate. Considerable depth of investigation is a highly desirable factor in well logging because of the heterogeneity of rocks making shallow observations unrepresentative, and therefore inaccurate as a representation of the whole mass of rock penetrated.

There are available at the present time only a very few types of influences by which desirable observations as discussed above may be made. Obviously, the magnetic and electric fluxes are not available for consideration in connection with cased wells, and the electric flux is unusable when investigating non-conducting material. The observation of the heat flux is familiar in the art of well logging and has patently the disadvantage that such observations are slow if one desires a considerable depth of investigation, The transmission of observable infrared and ultraviolet radiations is excluded because of the opacity of substances generally present in the earth and in bore holes. The gravitational flux has satisfactory properties, and, in principle, could be measured. But no known means of measuring it for well logging purposes has been found.

In attacking the above problem, seeking for a method of specific recognition of material in the circumstances of a bore hole penetrating the rock strata of the earth, it has been discovered that there are apparent specific properties of atomic nuclei corresponding with energy transitions in those nuclei. These transitions may evidence themselves in a variety of ways, such as:

(a) The emission of radiant energy through space.

(b) The absorption of a particular amount of energy from a bombarding particle or quantum.

(c) A specific energy threshold or a plurality of energy thresholds of susceptibility of the nuclei to certain classes of nuclear change, which may be caused by bombarding corpuscles or quanta.

It has been discovered that in all branches of molecular, atomic, and sub-atomic physics, one may generally predict that if a specific energy transition is possible in a quantized system, there will be a resonance effect, specifically affecting bombarding particles or quanta possessing energy (either kinetic or potential) in the close vicinity of the amount required to produce a quantized transition. The discovery of the details of quantization of nuclei of atoms still waits for extensive experimental and theoretical work. Limited experimental evidence has already brought support to the conviction 'which exists in the minds of all nuclear physicists to the effect that nuclei will surely be found to be quantized systems. In some instances energy thresholds of various kinds have already been determined for nuclei. For example, the photoneutron threshold is now known experimentally through the study of its inverse process, capture, by Kubischek and Dancoff.

A specific energy threshold at 20 megavolts has been found for the system comprising 4- nucleons (2 protons and 2 neutrons). Sundry isomeric transitions correspond ing with highly forbidden transformations of the arrangements of nucleons have been found experimentally and can be considered as additional evidence of the truth and experimental significance of the general conclusion that nuclear matter exists in quantized energy states.

In an effort to make use of the foregoing general conclusion, it has been discovered that only two classes of radiation appear to exist which react with nuclear matter appreciably and can be arranged conveniently for the observation of quantized energy levels of nuclei. These classes of radiation are the photon or electromagnetic class, and the corpuscular class comprising neutrons. Other particles (charged) in general do not penetrate the coulomb field of force surrounding a nucleus at energy falling in the range of possible excitation processes of common'nuclei. Such excitation processes are typically expected for light nuclei in the vicinity of 1 million electron vol-ts.

Charged particles lack action through a distance as defined herein. Therefore, corpuscular radiations of the charged variety would, in principle, not be particularly useful for investigation of the quantized levels of nuclei. Of the classes of radiation which have been suggested, the only one which has been discovered which has a favorable ratio for the amount of inter-action which it undergoes with nuclear matter, as compared with the energy transistions effected in the progress of the radiation by circumstances arising outside the nuclei of atoms, is the neutron. The photon reacts extensively with orbital electrons, and has only a very small cross section (target probability) for interactions with nuclei as such, There is furthermore an additional reaction of photons which becomes prominent above 2 electron megavolts, and which, in the range above 2 electron megavolts results in materialization of electron-positron pairs. This materialization, though influenced by the presence in the near vicinity of the nuclear field of force, does not represent a specific or identifying characteristic of particular nuclei, but is a general characteristic of all nuclei, more prominent for the nuclei of heavy elements like lead and less prominent for the nuclei of light elements such as aluminum. For the above listed reasons, there appear to be only a few especially simple reactions caused by photons which might be of any use. One might find it desirable to observe the neutrons released from nuclei by photons, since there is, for such nuclear photo-neutrons, a specific threshold of energy for each nuclear species (element or isotope thereof). One might also investigate the unmodified Compton scattering of energetic photon radiations in the hope of finding some slightly modified lines which suffered loss of energy by interaction with nuclei. This possibility is somewhat favored by the fact that the otherwise much stronger modified Compton scattering radiation is rapidly eliminated from the flux by absorption.

On the other hand, the interaction of neutrons with the outside parts of the atom is o small that the direct production of ion-pairs by neutrons is found to occur on an average of only about one time per meter of ordinary atmospheric air for a neutron possessing a kinetic energy of five million electron volts. The liberation of energy by neutrons in air therefore amounts to less than onethousandth of 1% per meter of air traversed for energy liberated by processes involving the outside portions of the atoms found in the air. A distance of travel in air which would result in an average loss of energy by reaction with outside parts of the atoms of less than 1%, would, nevertheless, result in total absorption of the neutrons, and all their energy, by reaction with the nuclei of the atoms contained in air. Even so, many of the reactions which neutrons undergo, which occur between neutrons and nuclei of the matter, are not highly specific, nor do they aid in any refined efforts to identify such matter. Among the unidentifying nuclear reactions one may name, for example, conservative ballistic nuclear scattering of neutrons, that is, conservative of total kinetic energy. This process is specifically different to an extreme degree only in the case of very light elements such as hydrogen and helium. The average nature of other matter contained in the rocks is sufficiently alike in this respect that the main possibility of use of the property of conservative ballistic nuclear scattering of neutrons is to observe differences in the propagation of neutrons through the rock which enable conclusions regarding the presence of hydrogen to be made. This effect is already made use of, and there exist a considerable number of US. patents and other published descriptions bearing on this subject. Among these patents are No. 2,308,361, No. 2,220,509, and No. 2,349,712. The broad class under which these previously named inventions fall corresponds with a patent issued to John C. Bender, No. 2,133,776.

The theory of detection of hydrogen by conservative ballistic nuclear scattering is treated in an article Written by Robert E. Fearon and published in the June 1949, issue of Nucleonics, entitled Neutron Well Logging.

The above theory finds general application in pursuing this method, and FIGURES 1 and 2 more particularly set forth the details of arrangements through which these general concepts find specific application to the problem set forth above.

Referring to these figures there is illustrated in application of this invention to a well surveying system. In FIGURE 1 there is shown schematically a drill hole It) which may or may not be cased. Disposed in the drill hole and adapted to be raised or lowered therein is a housing 11 supported by a cable 12. Cable 12 comprises at least one electrical conductor connecting the electrical apparatus within the housing 11 to apparatus located adjacent the mouth of the drill hole 19'. The apparatus on the surface of the earth consists of a measuring wheel 13 over which the cable 12 passes and a winch or drum 14 on which the cable is wound, or from which it is unwound, when the housing 11 is raised or lowered in the drill hole 10. Conductors are connected to the cable 12 by means of slip rings 15 and brushes 16- carried on one end of drum 14. These conductors lead to an amplifier 17. Amplifier 17 is conventional audio amplifier having a flat frequency response. The output of amplifier 17 is conducted to a pulse sharper 18, the purpose of which is to insure the delivery of square topped waves of constant height to an integrator 19. Integrator 19 is adapted to receive the aforementioned pulses and generate therefrom an electromotive force which is proportional to the average time-rate of occurrence of the pulses. This signal is delivered to the recorder 2% where it is recorded versus depth. The depth axis of the recorder is actuated by the shaft 21 which leads from a gear box 22, connecting through shaft 23 to the measuring wheel 13. The gear box 22 has adjustments to enable suitable choice of depth scales.

Referring specifically to FIGURE 2 a description of the contents of housing 11 will follow. It is to be understood that housing 11 will be constructed to withstand the pressures, and mechanical and thermal abuses encountered in surveying a deep bore hole and yet provide adequate space within it to house the necessary apparatus and permit the transmission of radiation through it.

In the bottom portion of housing 11 there is located a radiation source 24 which may be surrounded by a radiation filtering material 25. This radiation source may take various forms which will be described in detail later in the specification. Above the filtering material 25 and lying between the source of radiation and a radiation detector 26, there is a region of space which may be occupied by suitable materials or left vacant determined by considerations explained as the description progresses.

The detector 26 is of the type which will detect neutrons as a result of the production of prominent bursts of ionization therein, caused by rapid movements of heavy charged particles such as protons, alpha particles, etc., set in motion by the neutrons. The bursts of ionization are very quickly collected in the detector 26. These bursts are registered as electrical pulses and resolved timewise from other or smaller pulses which may occur almost concurrently. The detector 26 is so designed and so operated that the magnitude of the electrical pulse released from the collection of a specified amount of electrical charge will always be quite accurately proportional to the amount of the electrical charge collected and substantially independent of the path in the detector along which the burst of ionization occurred.

The current corresponding to a pulse, flowing in the electrode circuit which includes conductor 27, resistance 28, battery 2% and conductor 30, produces a voltage pulse across the resistance that is of the form illustrated at a. The pulse produced across the resistance 28 is impressed through the condenser 31 upon the input of an amplifier 32. As shown at b the pulse has suffered negligible loss and no distortion in passing through the condenser 31. The amplified pulse, illustrated at c, has been inverted in polarity but otherwise faithfully reproduced. It is then conducted to the pulse height distribution analyzer 33. Here only those pulses whose magnitude fall within a prescribed range, such as illustrated at d and designated by e, are accepted and transmitted. Other pulses such as are illustrated at f and g are not accepted and trans mitted. T h'ose pulses which are accepted and transmitted are delivered to an amplifier 34. Amplifier 34 is one having a flat frequency response extending upward to the highest frequency required to faithfully amplify the pulse delivered to it in a manner shown at h. The output signal from the amplifier 34 is fed into a scaling circuit 35 which, in a known manner, delivers pulses as illustrated at i, the number of which, occurring in a given time is less by a constant factor than the number received in the same interval of time. The output of the scaling circuit is fed into a shaper 36 which transforms the pulse into the shape illustrated at j. The shaper 36 may take the form of a powdered iron core transformer. The signal from the transformer is then fed into impedance matching means 37, such as a cathode follower, which faithfully reproduces the voltage wave as illustrated at k. The impedance matching means 37 introduces the signal into the transmission line contained within the cable 12 for the purpose of transmitting it to the surface.

It is to be understood that all elements within the housing 11 which require power may be powered in a conventional manner as taught in the art by means such as batteries or rectified alternating current. Batteries which very satisfactorily fulfill the temperature require ments in hot Wells are the zinc, potassium hydroxide, mercuric oxide cells.

Again referring to FIGURE 1, the signals transmitted to the surface by means of cable 12 are taken therefrom by means of slip rings 15 and brushes 16 and are con ducted to the amplifier as pulses, one of which is illustrated at I. These amplified pulses are received by a pulse shaper 18 which modifies their form in the manner illustrated at 0. The pulse illustrated at will always have a fixed square form with a fixed height in and a fixed width n. These substantially square pulses are then fed into the integrating circuit which delivers the signal to the recorder 20, as has been previously described. The integrating circuit thus produces a time-dependent voltage Wave such as shown at p. When this signal is impressed on the recorder, which has been coordinated with depth, a curve will be drawn as shown in FIGURE 3. This curve has as its ordinate depth in the bore hole and as its abscissa a function of an intensity of received radiation, or of a plurality, or combination of intensities. These intensities may be combined by adding, subtracting, or dividing in any desired manner, or may be otherwise mathematically combined. The manner of combination is suitable to specifically indicate, or be especially sensitive to, the presence of a particular substance in the region adjacent the bore hole.

Although no power supply has been shown in connection with the surface apparatus, it is to be understood that it will be powered in a conventional manner such as was pointed out in connection with the subsurface apparatus.

As can be understood from previous parts of this application, it is an object of this invention to measure only certain parts of an otherwise less in formative flux of scattered, diifuscd, or partially absorbed flux of neutrons, and to use data concerning the intensity of these dissected portions of the neutron flux as a means of obtaining more specific information regarding the nature of the substance by which the primary neutron flux is diffused, scattered or absorbed. Quite naturally, therefore, it may be seen that the measurement proposed herein is more difficult in certain particulars than those called for by the discoveries of the prior art. For example, the requirement that there be, within the interval of time in which a measurement is performed, a statistically sufficient number of processes to produce an accurate observation of the average rate of occurrence of such processes, will be less satisfactorily met. This conclusion is derived from the proposition that this discovery concerns itself in each instance with a measurement of only a part of the neutron radiation. Probable error in the measurement of any radiation is decreased when adequate intensity prevails, the percentage probable error in general being inversely proportional to the square root of the intensity. For illustration, therefore, if there are neutrons composing an energy spectrum uniformly distributed from zero to five million electron volts, and it is desired to observe that portion of the energy spectrum lying between three thousand four hundred electron kilovolts, and three thousand five hundred electron kilovolts, the percentage probable error of such a measurement will be approximately seven times worse than it would be if the measurement had used all the neutrons. It follows, therefore, that strong fluxes of neutrons are needed to practice this well logging method. It likewise follows that, if the neutrons are to be undirected, there is need that they be generated in some isotropic nuclear process.

The strength of the neutron source required will be related to the economic requirement of logging speed,

ho rified i0 and the error which is considered tolerable in a given case, by the formula where S is logging speed in feet per hour.

6 is the fraction of the total flux of fast neutrons incident on the detector from all directions.

p is the intensity of primary neutrons, in units of 10" per second at 8 million electron volts from the source.

Error of :L5% has been assumed (for spacings, source to detector in the range 10"-18).

If the undirected flux of neutrons is monoenergetic, the chosen isotropic nuclear process must of necessity be one in which a constant amount of energy is liberated into the propulsion of the neutron every time the said process occurs. It also follows that if the primary neutron flux is to be of a penetrating nature, the neutrons generated therein must be of relatively high energy. If helium is to :be considered as a recoiling substance in a detector of neutron radiation, neutrons cannot be employed which have energies high enough to undergo an inelastic collision with helium. If high energy neutrons are employed, a more complex and ambiguous distribution of recoil energies will occur. To illustrate the ambiguity brought about in such a case, consider, for example, the problem of determining the presence of fast neutrons having a kinetic energy of one million electron volts. If the incident flux of fast neutrons which impinges upon helium contains also some neutrons having energy of 21 million electron volts, absorption of the resonance energy of 20 million electron volts will occur, sometimes generating 1 million electron volt neutrons, a fraction of which will be measured, and will be indicated in a manner indistinguishable from the effect caused by the neutrons which had one million electron volts in the first place. This result is altogether avoided if no neutrons having energies equal to, or greater than, 20 million electron volts are emitted from the source.

The requirement that very many neutrons be available is met only if there be sufiicient energy dissipated per unit of time by whatever bombardment produces the neutrons. There are tWo ways of producing an adequate flux of neutrons within the space available for a well logging radiation source. One of these ways to provide a mixture of beryllium with an alpha-ray emitter of a sufiicient degree of activity per unit volume. This achievement is favored if such an alpha-ray emitter (a) has a short half life. This increases the rate of energy liberation per unit weight and per unit volume, other things being equal.

(b) is a parent of a series which gets into equilibrium sufficiently quickly, and which comprises sufficiently numerousialpha-emitting daughter products in the series.

(0) has large energy per alpha particle.

(d) has a low atomic weight.

Of the above 4 conditions, only the first 3 are at all possible since there are fundamentally serious theoretical dilficulties which appear to absolutely prohibit the fulfillment of any expectations of consequence with respect to item (d). It may be said further that, with only one exception, which is not of any importance to the uses of this invention, the expectation of the present theory is fully confirmed with respect to the above stated conclusion pertaining to item (d). Of the thousand or so isotopes that are now known, only one having atomic number less than 81, or an atomic weight less than 208, Samarium, is found to emit alpha particles. Furthermore, this one exception emits alpha particles of such a low energy, and emits so few of them per unit weight of material per unit time, that it would be utterly useless to consider it as a practical source of bombardment to generate neutrons from beryllium.

-It is, there fore, perfectly clear that the considerations of the first three items are those which prevail in attempting to arrange a bountiful source of neutrons made of a mixture of beryllium with alpha-ray emitting substance. The particular merits of an arrangement containing an adequate quantity of actinium, or actinium salt, mixed with beryllium have been taken note of in United States Patent No. 2,515,502 and will not be reviewed extensively here, except to note the fact that one can, with actinium, crowd 200 times as much neutron-emitting power into a given space as can be done with radium-beryllium mixtures. Polonium would be suitable substance for a concentrated source of neutrons. Thorium X would be suitable, and would enable the design of very powerful neutron sources with limited available space. Numerous other effective choices of powerful neutron sources are possible, and will be apparent to those familiar with the art, upon consideration of the previously outlined conditions for the design of such powerful neutron-emitting sources.

Returning to the general question of powerful and intense sources of neutrons in a broader sense, it is apparent that in the limited space within a well one is at liberty to consider electrically or electro-magnetically accelerated ion beams impinging upon suitable target material provided they do not require particle energy in the beam that is too high to be conveniently producible (considering insulation problems, etc.) within the limited space available. It is clear therefore, that reactions between ionic beam materials and suitable target substances are a matter of consequence to the practice of this invention with increasing emphasis in the case of those target reactions having a low threshold of energy per bombarding ionic particle for their onset.

As is well known in the art of designing RF. power supplies such as those used for television sets, it is feasible to produce electrical potential differences of the order of 20 thousand volts within a limited space, and insulated by very reasonable thicknesses of rubber or other high voltage insulation.

There are available for consideration two nuclear reactions which can be excited by ionic beams propelled by no greater electrical potential difference than 20 thousand volts. These reactions are:

(a) The bombardment of deuterium atoms by deuterium ions, or if preferred, bombardment of substances rich in deuterium atoms with moving deuterium ions.

(b) Bombardment of tritium atoms or molecules rich in tritium atoms with deuterium ions, or conversely, the equivalent process, bombardment of deuterium atoms, or substances rich in deuterium atoms by moving tritium ions.

This latter reaction is one especially favored for the practice of this invention, because of its large efficiency, and because of the extremely favorable way in which the efliciency of this reaction improves with electrical potential applied at very low electrical potential differences. The second of these reactions is also particularly favored because of the large self-energy, that is, conversion of mass into kinetic energy, by which it is characterized, amounting to approximately 17 million electron volts, or" which approximately 14.2 million are delivered to the neutron which is produced. Owing to the very large selfenergy to which reference has been made above, neutrons derived from this preferred target reaction at very low bombarding energies nevertheless have very great energy, and are substantially monoenergetic. The same things can be said, but to a lesser degree, in respect to the first named of the two described bombardment-s. In it, the self-energy is less, delivering only 2.5 million electron volts to the neutrons, and the efliciency of the reaction is much lower. Accordingly, smaller fluxes of neutrons would be available under like circumstances, and the neutrons would be less monoenergetic.

In FIGURE 4 of the drawings there is illustrated diagrammatically a neutron source of the type described above. This source can be used in the housing 11 to replace the source 24 shown in FIGURE 2.

A glass envelope 38 encloses electrodes 39 and 40. These electrodes may be formed of tantalum, uranium or zirconium. Electrode 40 may be a wire or a cylinder of suitable size. Electrode 39 is in the form of a concentric cylinder.

These electrodes are processed to introduce in them deuterium or tritium, or both. This is accomplished by supplying a suitable atmosphere of deuterium or tritium, or a mixture of these, under conditions which enable the electrodes to absorb these gases. Such conditions are produced by heating the electrodes or by conducting an electrical discharge between them as separate processes or both processes may be carried on concurrently. This conditioning of the electrodes is necessary in order that target atoms of deuterium or tritium may be situated in a suitable manner such that they will suffer collisions with bombarding ions. Tantalum, uranium and zirconium were selected as materials for the reason that they have the property of absorbing large quantities of deuterium and tritium.

Electrodes 39 and 40 are disposed in an atmosphere of deuterium gas, tritium gas, or a mixture of both at a pressure of from 1 to microns of mercury.

If it is desired to operate this neutron source as a deuterium-deuterium reactor, the electrodes will be conditioned with deuterium and the final filling atmosphere will be deuterium.

If it is desired to operate this source as a deuteriumtritium reactor, conditioning with deuterium may be followed by filling with tritium, or conversely conditioning with tritium and filling with deuterium may be used.

In both the above arrangements for producing the deuterium-tritium reaction, the substance in the electrodes will exchange with the filling atmosphere, causing the efficiency of the reaction to vary slowly during operation.

Stability of operation, with somewhat lower initial efiiciency is secured by conditioning the electrodes with a half and half mixture of deuterium and tritium and filling with the same mixture. Collisions in the target, in this case, are

(1) D on Zr No radiation.

(2) T on Zr No radiation.

(3) D on T 14.2 m.e.v. neutrons. (4) T on D 14.2 m.e.v. neutrons. (5) D on D 2.5 m.e.v. neutrons. (6) T on T Inefficient.

If the half and half mixture is used the sum of Reactions 3 and 4 would predominate about 50 to 1 over the process of Item 5 in number of neutrons emitted from these causes. Reaction 6 is ineflicient at low bombarding voltages.

Voltage is supplied to the electrodes 39 and 40 from the power supply 41 by means of conductors 42. A switch 43 is provided in one of the conductors 42. Switch 43 may be operated by the solenoid 44 which is energized through the conductor 45 that extends through the housing 11 to the surface of the earth.

The intensity of emission of neutrons will be augmented in increasing proportion as the electrical power delivered to the discharge is increased. The range of energies which will result will depend upon how the energy of the incident ion is divided between the neutron and the recoiling nucleus; this depends upon the direction of the neutron relative to that of the incident ion. Of the order of 10 neutrons per second can be secured from a discharge dissipating 500 watts of electrical energy, in the D-T reactor.

Where an extremely large flux of neutrons is desired it is expedient to raise the bombardment energy of the D-T reaction to a higher value. This is particularly good sot-rest) because the efficiency of the -D-T reaction rises rapidly as bombardment energies of the order of 100 kilovolts are attained. With the space available in a well logging instrument and with the new insulating material-s, it is entirely feasible to build electronic voltage generators with output of the order of 100 kilovolts. An example of such a generator would be a high frequency Cockroft- Walton type of apparatus. Particular stress is laid on the high frequency feature in order that the condensers in the circuit would fit in the well logging instrument.

Still another type of neutron source is illustrated diagrammatically in FIGURE 5. This source produces by the D-D reaction neutrons having energies of approximately 2.5 million electron volts as described in connection with the source illustrated in FIGURE 4. By employing the -D-T reaction, neutrons having energies of approximately 14.2 million electron volts can be produced. This apparatus is also adapted to produce 17 million electron volt gamma rays by the lithium-proton reaction.

Referring to FIGURE a substantially cylindrical housing 46 encloses a central electrode 47, a first screen 48, and a second screen 49. These elements are disposed in an atmosphere which consists of an isotop of hydrogen or a mixture of such isotopes. Potentials are placed between the elements by the voltage sources 50, 51, and 52. The housing is grounded as shown at 53. The voltage source 50 impresses a potential between the second screen 49 and the housing 46. The screen 49 is made sufiiciently negative that the electric field perpendicular to the inside surface of the housing 4-6 is nowhere positive. The voltage source 51, impresses a potential between the central electrode 47 and the first screen 48. This voltage source serves to strike a low pressure arc to produce and make available positive ions. The voltage source 52 impresses a potential between the screen 48 and the housing 46. This potential produces an accelerating electric field which acts upon positive ions which escape through the screen 48 and which im pinge upon a thin layer of target substance 54 which is uniformly deposited on the inner surface of the housing 46. The target material may be formed of a diatomic compound of lithium and a suitable isotope of hydrogen.

The electrodes shown in FIGURE 5 are spaced from one another in a manner which is correlated with the pressure of the filling gas. The radial distance between elements 46 and 48 is made short compared to the mean free path of an electron in the ifilling gas at the prevailing pressure. The radial distance between elements 47 and 48, on the other hand, is chosen to exceed several times the electron mean free path in the chosen atmosphere. The purpose of these choices is to permit a selfsustaining low pressure are in the circuit of power source 51 and to forbid it in the circuit of power source 52 as a result of the short space between the electrodes 46 and 48. Any discharge between electrodes 46 and 48 will, therefore, be continuously dependent on replenishment of ions from the space incide of screen 48. Because the electric field between 46 and 48 can accept only positive ions from inside 48, electrons being repelled, the parasitic discharge in the space between electrodes 46 and 48 will be a positive ion airair, continuously replenishing its supply of ions by leakage through the holes in the screen 48. The positive ions leaking through the holes will impinge, in part, on outer screen wires of screen 49, which functions much as does a suppressor grid in a pentode vacuum tube. This outer screen serves to suppress the emergence into the electric field between elements 46 and 48 of electrons emitted by the target material 54. Were the suppressor screen not present, the bombardment of the target with positive ions, and with light and ultraviolet radiation, would cause a copious emission of electrons, which, falling through the electric field between electrodes 46 and 43, would waste i4 the electrical energy of power source 52, which was intended to do work exclusively on the positive ions.

The voltage supplied by source 52 controls the bombarding energy of the ions incident upon the target 54. The choice of this voltage must be varied to suit the requirements of the problem. For example, the 13-1) reaction has a zero threshold, but a more copious flow of neutrons will occur as the voltage rises. The supply of neutrons from the D D reaction is observable, and would have some uses at ten thousand volts, but would be very much better at 20,000 volts or more. However, as has been stated earlier, the neutrons will not be as strictly monoenergetic, that is, the energy range will be broader as the bombarding energy rises.

The D-T reaction also has a zero voltage threshold, but becomes importantly ethcient at very low voltages. The eiliciency of both the D-D reaction and the D-T reaction is satisfactory below fifty thousand volts for well logging purposes. Higher voltages will, however, produce a more copious fiow of neutrons, especially in the case of the 13-1) reaction.

The lithium-proton reaction has a resonance in the neighborhood of 450,000 volts for the production of the 17 million electron volt gamma rays, but like the other reactions, D-D and D-T, commences at very low voltages.

For the D-D reaction, lithium deuteride would be the target, and the filling would be deuterium. For the 13-1 reaction the target could be lithium tritide and the filling deuterium, or the target could be lithium deuteride and the filling composed of tritium. These two cases would have an instability due to exchange between the atmosphere and the target, exactly analogous to the instability caused by the same consideration in the case of the tan- Italum or zirconium source. The instability referred to above may be corrected by using a target composed equally of LiD and LiT molecules, and a gas composed equally of deuterium and tritium. For the production of the lithium-proton reaction, a target of lithium hydride will be used, and a filling of ordinary hydrogen. Voltages and spacings will have to be adjusted for these various fillings, and the pressures will have to be adjusted because the mean free path of electrons is not exactly the same in the three isotopes of hydrogen at the same pressures.

In FIGURE 6 there is illustrated a modified form of the neutron source shown in FIGURE 5. Its principle of operation is the same. Element 55 corresponds to element 47 in FIGURE 5. The housing 56 corresponds to element 43 and space charge electrode 57 corresponds with the outer screen 49. The anode 58 corresponds with the housing 46. Similarly a large space exists between elements 55 and 56 and a small space exists between elements 56 and 58. Similarly the large space exceeds by several times the mean free path of the electrons in the filling gas at the prevailing pressure, whereas the short space is chosen less than the mean free path of the electrons.

We claim:

1. A fast neutron source that comprises a housing, a target material formed of a compound of lithium with a heavy isotope of hydrogen in said housing, a source of ions of the other heavy isotope of hydrogen also in said housing, and means for accelerating said ions to bombard said target.

2. A fast neutron source that comprises a housing, a target containing a substantial amount of a plurality of heavy isotopes of hydrogen in said housing, a source of ions of a mixture of heavy isotopes of hydrogen also in said housing, and means for accelerating said ions to bombard said target to produce neutrons.

3. A neutron source that comprises a housing, a gas confined under static pressure in said housing that contains a substantial proportion of at least one heavy isotops of hydrogen, electrostatic means pervious to said gas for dividing said gas electrostatically into two regions,

electrode means disposed in one of said regions and spaced apart far relative to the mean free path of electrons in said gas, a first voltage source connected to said electrode means to ionize said gas in said one region, a target containing a substantial amount of at least one heavy isotope of hydrogen disposed in the other of said regions and spaced from said electrostatic means by distance short relative to the mean free path of electrons and ions in said gas, a substantial part of the hydrogen content of said target being of a different heavy isotope of hydro gen than a substantial part of the hydrogen of said gas, and a second voltage source connected to apply voltage between said electrostatic means and said target to accelerate ions from said one region through said second region to bombard said target without substantial further ionization in said other region.

4. A neutron source that comprises a housing, a gas confined under static pressure in said housing that contains a substantial proportion of at least one heavy isotope of hydrogen, a first electrostatic means pervious to said gas for dividing said gas electrostatically into two regions, electrode means disposed in one of said regions and spaced apart far relative to the mean free path of electrons in said gas, a first voltage source connected to said electrode means :to ionize said gas in said one region, a target containing a substantial amount of at least one heavy isotope of hydrogen disposed in the other of said regions and spaced from said electrostatic means by distance short relative to the mean free path of electrons and ions in said gas, a substantial part of the hydrogen content of said target being of a ditferent heavy isotope of hydrogen than a substantial part of the hydrogen of said gas, a second voltage source connected to apply voltage between said electrostatic means and said target with said target relatively negative to accelerate ions from said one region through said second region to bombard said target Without substantial further ionization in said other region, a second electrostatic means pervious to said gas disposed between said first electrostatic means and said target, and a third voltage source connected to apply voltage between said second electrostatic means and said target with said target relatively positive to suppress electron emission from said target.

5. A neutron source that comprises a housing, a gas confined under static pressure in said housing that contains a substantial proportion of at least one heavy isotope of hydrogen, electrostatic means pervious to said gas for dividing said gas electrostatically into two regions, an electrode disposed in one of said regions and spaced apart from said electrostatic means far relative to the mean free path of electrons in said gas, a first voltage source connected between said electrode and said electrostatic means to ionize said gas in said one region, a target containing a substantial amount of at least one heavy isotope of hydrogen disposed in the other of said regions and spaced from said electrostatic means by distance short relative to the mean free path of electrons and ions in said gas, a substantial part of the hydrogen content of said target being of a difiFerent heavy isotope of hydrogen than a substantial part of the hydrogen of said gas, and a second voltage source connected between said electrostatic means and said target to accelerate ions from said one region through said second region to bombard said target without substantial further ionization in said other region.

6. A fast neutron source that comprises a housing, a target containing deuterium and tritium disposed within said housing, gas containing deuterium and tritium confined within said housing, means for ionizing said gas, a voltage source of the order of 100 kilovolts, and means for utilizing said voltage source for accelerating the ions produced to bombard said target, the relative amounts of deuterium and tritium in said gas and said target being such as to remain substantially the same during operation.

7. A source of neutrons for radioactivity well logging that comprises a housing, deuterium gas confined within said housing under static pressure, means for ionizing said deuterium gas, and electrical means for accelerating deuterium ions soproduced against a tritium target.

8. In radioactivity well logging, a method of bombarding the formations surrounding a drill hole with neutrons that comprises confining deuterium gas under static pressure, ionizing said confined deuterium gas, and accelerating the resultant deuterium ions by an electric field against a tritium target.

9. In radioactivity well logging, a method of bombarding the formation surrounding a drill hole with neutrons that comprises confining deuterium gas under static pressure, accelerating electrons, ionizing said confined deuterium gas with said accelerated electrons, and accelerating the resultant deuterium ions by an electric field against a tritium target, whereby neutrons of 14 m.e.v. energy are produced.

10. A source of neutrons for radioactivity well logging that comprises a housing, deuterium gas at a static low pressure, means for accelerating electrons within said deuterium gas, to ionize said deuterium gas, and electrical means for accelerating the resultant deuterium ions against a tritium target to produce 14 m.e.v. neutrons.

11. A source of neutrons comprising a chamber, a gaseous atmosphere comprised of at least two hydrogen isotopes each having at least one neutron confined within said chamber under static pressure, means for ionizing said gaseous hydrogen isotope, and electrical means for accelerating hydrogen isotope ions so produced against a target containing at least two hydrogen isotopes having at least one neutron, the relative amounts of said hydrogen isotopes in said atmosphere and said target being such as to remain substantially constant during operation.

12. A source of neutrons comprising a chamber, a gaseous atmosphere comprised of at least two hydrogen isotopes each having at least one neutron confined Within said chamber under static pressure, means for accelerating electrons Within said gaseous hydrogen isotopes to ionize said gaseous hydrogen isotopes, and electrical means for accelerating the resultant hydrogen isotope ions against a target containing atmosphere comprised of at least two hydrogen isotopes having at least one neutron, the relative amounts of said hydrogen isotopes in said atmosphere and said target being such as to remain substantially constant during operation.

13 In a neutron source the combination of a chamber, deuterium and tritium gas under static pressure confined within said chamber, means located at one end of said chamber for forming ions in said gas, a target containing hydrogen isotopes having at least one neutron supported in opposed relation to said ion forming means, means for impressing a high negative voltage on said target for attracting ions formed in said ion forming means toward said target, ion focusing means including an anode located between said ion forming means and said target for forming into a beam said ions attracted toward said target, and high voltage envelope means located adjacent said target for suppressing electrons emitted from said target and for reducing the distance between said high voltage and said chamber and anode the relative amounts of said deuterium and tritium in said gas and of said hydrogen isotopes in said target being such as to remain substantially the same during operation.

14. In a neutron source the combination of a chamber, deuterium and tritium gas, under static pressure confined within said chamber; means located at one end of said chamber for forming ions in said gas; a target containing hydrogen isotopes having at least one neutron supported in opposed relation to said ion forming means, means for impressing a high negative potential on said target for attracting ions formed by said ion forming means; an anode located between said ion forming means and said target and having a central aperture, said anode dividing each chamber into a first and second area, said first area containing said ion forming means, said second area containing said target and said second named means; said first and second area being connected through said anode aperture; high voltage envelope means located in said second area for suppressing electrons emitted from said target, and for reducing the distance between said high potential and said chamber and anode the relative amounts of deuterium and tritium in said gas and of said isotopes in said target being such as to remain substantially the same during operation.

15. A fast neutron source that comprises a housing, a target containing a substantial amount of a heavy isotope of hydrogen disposed within said housing, gas containing a substantial proportion of the other heavy isotope of hydrogen confined under static pressure Within said housing, means for ionizing said gas, and means for accelerating the ions produced thereby to bombard said target.

16. An apparatus for producing a neutron log of a well that comprises a source of fast neutrons, said fast neutron source comprising a housing, a target containing a substantial amount of a heavy isotope of hydrogen disposed within said housing, gas containing a substantial proportion of the other heavy isotope of hydrogen also disposed within said housing, means for ionizing said gas, means for accelerating the ions produced thereby to bombard said target; means for traversing the well with said source to effect bombardment of the formations with fast neu- 18 trons; means disposed a fixed distance from said source" and adapted for movement therewith for detecting radia= tions from the said formations occasioned by said bombardment; means for recording signals resulting from sai detection in correlation with the depth at which detection occurred; and means for transmitting the signals from said detwting means to said recording means.

References Cited in the file of this patent UNITED STATES PATENTS 2,161,985 Szilard June 13, 1939 2,211,668 Penning Aug. 13, 1940 2,220,509 Brons Nov. 5, 1940 2,240,914 Schutze May 6, 1941 2,251,190 Kallmann July 29, 1941 2,302,247 Neufeld Nov. 17, 1942 2,483,139 Herzog Sept. 27, 1949 2,489,436 Salisbury Nov. 29, 1949 OTHER REFERENCES Bretscher et al.: Physical Review, vol. 73, No. 8, April 15, 1948, pp. 815 to 821.

Bretscher et al.: Physical Review, vol. 75, No. 8, April 15, 1949, pp. 1154 to 1160.

Baker et al.: Atomic Energy Commission Document IAMS-ll, declassified August 26, 1948.

Hanson et al.: Review of Modern Physics, vol. 21, No. 4, October 1949, pages 639 to 641 relied on.

UNITED STATES PATENT OFFICE CERTIFICATE OF CORRECTION Patent N00 3,071 ,690 January 1 1963 Robert E0 Fearon et a1,

It is hereby certified that error appears in the above numbered patent requiring correction and that the said Letters Patent should read as corrected below.

Column 3 line 18, for "and evaluates other variable" read an evaluates other variables column 7 line 75, after "is" insert a column 8, line 2, for "sharper" read shaper column 9, line 40, for "in formative" read informative column 13, line 24, for "-isotop read isotope line 59, for "incide" read inside Signed and sealed this 27th day of August 19630 (SEAL) Attest:

DAVID L. LADD Commissioner of Patents ERNEST W SWIDER Attesting Officer UNITED STATES PATENT OFFICE CERTIFICATE OF CORRECTION Patent No., 3,071,690 January 1 1963 Robert E0 Fearon et al,

It is hereby certified that error appears in the above numbered patent requiring correction and that the said Letters Patent should read as corrected below.

Column 3, line 18, for "and evaluates other variable" read an evaluates other variables column 7, line 75, after "is" insert a -g column 8, line 2, for "sharper" read shaper column 9, line 40, for "in formative" read informative column 13, line 24, for "-isotop" read isotope line 59, for "incide" read inside Signed and sealed this 27th day of August 1963.,

(SEAL) Attest:

ERNEST w. SWIDER VI ADD Attesting Officer Commissioner of Patents 

3. A NEUTRON SOURCE THAT COMPRISES A HOUSING, A GAS CONFINED UNDER STATIC PRESSURE IN SAID HOUSING THAT CONTAINS A SUBSTANTIAL PROPORTION OF AT LEAST ONE HEAVY ISOTOPE OF HYDROGEN, ELECTROSTATIC MEANS PERVIOUS TO SAID GAS FOR DIVIDING SAID GAS ELECTROSTATICALLY INTO TWO REGIONS, ELECTRODE MEANS DISPOSED IN ONE OF SAID REGIONS AND SPACED APART FAR RELATIVE TO THE MEAN FREE PATH OF ELECTRONS IN SAID GAS, A FIRST VOLTAGE SOURCE CONNECTED TO SAID ELECTRODE MEANS TO IONIZE SAID GAS IN SAID ONE REGION, A TARGET CONTAINING A SUBSTANTIAL AMOUNT OF AT LEAST ONE HEAVY ISOTOPE OF HYDROGEN DISPOSED IN THE OTHER OF SAID REGIONS AND SPACED FROM SAID ELECTROSTATIC MEANS BY DISTANCE SHORT RELATIVE TO THE MEAN FREE PATH OF ELECTRONS AND IONS IN 